U.S. patent application number 11/384002 was filed with the patent office on 2007-07-05 for coupled and non-coupled opto-electronic oscillators with enhanced performance.
Invention is credited to Danny Eliyahu, Dmitri A. Kossakovski, Lutfollah Maleki, Ismail Tolga Yilmaz.
Application Number | 20070153289 11/384002 |
Document ID | / |
Family ID | 36992479 |
Filed Date | 2007-07-05 |
United States Patent
Application |
20070153289 |
Kind Code |
A1 |
Yilmaz; Ismail Tolga ; et
al. |
July 5, 2007 |
Coupled and non-coupled opto-electronic oscillators with enhanced
performance
Abstract
This application describes coupled and non-coupled
opto-electronic oscillators with enhanced performance. Coupled OEOs
implement a dispersion compensation mechanism to reduce
dispersion-induced optical loss, a polarization control mechanism
to reduce polarization-dependent optical loss, or a combination of
the dispersion compensation mechanism and the polarization control
mechanism to enhance the oscillator performance.
Inventors: |
Yilmaz; Ismail Tolga;
(Oviedo, FL) ; Eliyahu; Danny; (Pasadena, CA)
; Kossakovski; Dmitri A.; (South Pasadena, CA) ;
Maleki; Lutfollah; (Pasadena, CA) |
Correspondence
Address: |
FISH & RICHARDSON, PC
P.O. BOX 1022
MINNEAPOLIS
MN
55440-1022
US
|
Family ID: |
36992479 |
Appl. No.: |
11/384002 |
Filed: |
March 17, 2006 |
Related U.S. Patent Documents
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Application
Number |
Filing Date |
Patent Number |
|
|
60756601 |
Jan 4, 2006 |
|
|
|
Current U.S.
Class: |
356/464 |
Current CPC
Class: |
H01S 5/50 20130101; H01S
2301/08 20130101; H01S 5/1071 20130101; G01C 19/72 20130101; H01S
3/06791 20130101; H01S 3/06725 20130101; H01S 3/1109 20130101; H01S
3/1061 20130101; H01S 3/08036 20130101 |
Class at
Publication: |
356/464 |
International
Class: |
G01C 19/72 20060101
G01C019/72 |
Claims
1. A device, comprising: a ring laser comprising an optical ring
which comprises at least one optical gain medium operable to
produce laser light; an optical modulator coupled in the optical
ring and operable to modulate the laser light in response to a
control signal to produce a modulated laser beam; an
opto-electronic feedback loop comprising an optical portion
operable to receive a portion of light from the ring laser, a
photodetector operable to convert the received portion of light
into a detector signal, and an electrical portion operable to
produce the control signal from the detector signal; and a
dispersion compensation element coupled in the optical ring and
operable to compensate for optical dispersion in the optical
ring.
2. The device as in claim 1, wherein the dispersion compensation
element comprises a dispersion compensated fiber.
3. The device as in claim 1, wherein the dispersion compensation
element comprises a dispersion shifted fiber.
4. The device as in claim 1, wherein the dispersion compensation
element comprises a fiber Bragg grating.
5. The device as in claim 1, further comprising a polarization
control unit coupled in the optical ring and operable to control a
polarization of the laser light.
6. The device as in claim 1, wherein the optical ring includes
polarization maintaining fiber which controls a polarization of the
laser light.
7. The device in claim 1, further comprising an optical resonator
in the optical ring.
8. The device as in claim 1, further comprising: an optical
polarization beam splitter coupled in the optical ring to direct
light received from the optical ring into a first light beam; a
45-degree Faraday rotator to receive and transmits the first light
beam; a reflective unit to reflect the first light beam transmitted
through the Faraday rotator back to the optical polarization beam
splitter by transmitting through the Faraday rotator for a second
time; and a fiber delay line between an optical path between the
optical polarization beam splitter and the reflective unit to
transport light, wherein the optical polarization beam splitter is
coupled to the optical ring to direct light reflected back from the
reflective unit into the optical ring.
9. The device as in claim 8, wherein the reflective unit is a
mirror.
10. The device as in claim 8, wherein the reflective unit comprises
a fiber Bragg grating.
11. The device as in claim 1, further comprising: an optical
splitter to split the received portion of light from the ring laser
into a first beam and a second beam; a first optical delay path to
receive the first beam; a second optical delay path to receive the
second beam, wherein the first and second optical paths have
different optical delays, wherein the photodetector is coupled to
receive the first and second beams, at orthogonal polarizations,
from the first and second optical delay paths to produce the
detector signal.
12. A method, comprising: selecting a length of an optical ring
that generates laser light in a coupled opto-electronic oscillator
(COEO) which further comprises an opto-electronic feedback loop
coupled to the ring to produce a desired separation between a
carrier frequency generated by the COEO and a first spurious mode
generated by the COEO; and using a dispersion compensation element
in the ring to negate optical dispersion in the ring to reduce
phase noise of the COEO below an acceptable level.
13. The method as in claim 12, further comprising: controlling a
polarization of the laser light in the optical ring.
14. A device, comprising: an optical loop which comprises at least
one optical gain medium operable to produce laser light; an optical
modulator coupled in the optical loop and operable to modulate the
laser light in response to a control signal to produce modulated
laser light; an opto-electronic feedback loop comprising an optical
portion operable to receive a portion of the modulated laser light
from the optical loop, a photodetector operable to convert the
received portion into a detector signal, and an electrical portion
operable to produce the control signal from the detector signal; an
optical polarization beam splitter coupled in the optical loop to
direct light received from the optical loop into a first light
beam; a 45-degree Faraday rotator to receive and transmits the
first light beam; a reflective unit to reflect the first light beam
transmitted through the Faraday rotator back to the optical
polarization beam splitter by transmitting through the Faraday
rotator for a second time; and a fiber delay line between an
optical path between the optical polarization beam splitter and the
reflective unit to transport light, wherein the optical
polarization beam splitter is coupled to the optical loop to direct
light reflected back from the reflective unit into the optical
loop.
15. The device as in claim 14, wherein the optical loop is formed
from polarization maintaining fiber.
16. The device as in claim 14, further comprising: an optical
splitter to split the received portion of the laser light from the
optical loop into a first beam and a second beam; a first optical
delay path to receive the first beam; a second optical delay path
to receive the second beam, wherein the first and second optical
paths have different optical delays, wherein the photodetector is
coupled to receive the first and second beams, at orthogonal
polarizations, from the first and second optical delay paths to
produce the detector signal.
17. A device, comprising: a laser to produce CW laser light; an
optical modulator to modulate the CW laser light to produce
modulated laser light in response to an electrical control signal;
an optical splitter to receive at least a portion of the modulated
laser light and to split the received portion into a first beam and
a second beam; a first optical delay path to receive the first
beam; a second optical delay path to receive the second beam,
wherein the first and second optical paths have different optical
delays; a photodetector coupled to receive the first and second
beams, at orthogonal polarizations, from the first and second
optical delay paths to produce a detector signal; and an electrical
section operable to receive and process the detector signal to
produce the electrical control signal, wherein the electrical
section, the optical modulator, the optical splitter, the first and
second optical delay paths, and the photodetector form a part of a
closed opto-electronic feedback loop that is operable to have a
loop gain greater than the loop loss and to generate an oscillation
at a modulation frequency of the optical modulator.
Description
[0001] This application claims the benefits of the following two
U.S. Provisional Applications:
[0002] No. 60/622,963 entitled "COUPLED OPTO-ELECTRONIC OSCILLATORS
WITH DISPERSION COMPENSATION" and filed Mar. 17, 2005, and
[0003] No. 60/756,601 entitled "Dual Loop OEO/COEO Utilizing One
Photodetector" and filed Jan. 6, 2006.
[0004] The above two applications are incorporated by reference as
part of the specification of this application.
BACKGROUND
[0005] This application relates to optical and photonic devices for
various applications, such as optical, radio frequency (RF), and
microwave applications.
[0006] RF and microwave oscillators for generating signals in the
RF and microwave frequencies may be constructed as "hybrid" devices
by using both electronic and optical components to form
opto-electronic oscillators ("OEOs"). See, e.g., U.S. Pat. Nos.
5,723,856, 5,777,778, 5,929,430, and 6,567,436. Such an OEO
includes an electrically controllable optical modulator and at
least one active opto-electronic feedback loop that comprises an
optical part and an electrical part interconnected by a
photodetector. The opto-electronic feedback loop receives the
modulated optical output from the modulator and converted the
modulated optical output into an electrical signal which is applied
to control the modulator. The feedback loop produces a desired long
delay in the optical part of the loop to suppress phase noise and
feeds the converted electrical signal in phase to the modulator to
generate the optical modulation and generate and sustain an
electrical oscillation in RF or microwave frequencies when the
total loop gain of the active opto-electronic loop and any other
additional feedback loops exceeds the total loss. The generated
oscillating signals are tunable in frequency and can have narrow
spectral linewidths and low phase noise in comparison with the
signals produced by other RF and microwaves oscillators.
SUMMARY
[0007] This application describes coupled and non-coupled
opto-electronic oscillators with enhanced performance. Described
coupled opto-electronic oscillators implement a dispersion
compensation mechanism to reduce dispersion-induced optical loss, a
polarization control mechanism to reduce polarization-dependent
optical loss, or a combination of the dispersion compensation
mechanism and the polarization control mechanism to enhance the
oscillator performance. Some configurations of the coupled
opto-electronic oscillators described here may be used to shorten
the optical length of the optical loop and thus to reduce the
spurious modes in the generated electrical oscillation
spectrum.
[0008] In one implementation, a device is described to include a
ring laser comprising an optical ring which comprises at least one
optical gain medium operable to produce laser light at a laser
carrier frequency; an optical modulator coupled in the optical ring
and operable to modulate the laser light in response to a control
signal to produce a modulated laser beam; an opto-electronic
feedback loop comprising an optical portion operable to receive a
portion of light from the ring laser, a photodetector operable to
convert the received portion of light into a detector signal, and
an electrical portion operable to produce the control signal from
the detector signal; and a dispersion compensation element coupled
in the optical ring and operable to compensate for optical
dispersion in the optical ring.
[0009] In another implementation, a device is described to include
an optical loop which comprises at least one optical gain medium
operable to produce laser light; an optical modulator coupled in
the optical loop and operable to modulate the laser light in
response to a control signal to produce modulated laser light; and
an opto-electronic feedback loop comprising an optical portion
operable to receive a portion of the modulated laser light from the
optical loop, a photodetector operable to convert the received
portion into a detector signal, and an electrical portion operable
to produce the control signal from the detector signal. This device
further includes an optical polarization beam splitter coupled in
the optical loop to direct light received from the optical loop
into a first light beam; a 45-degree Faraday rotator to receive and
transmits the first light beam; a reflective unit to reflect the
first light beam transmitted through the Faraday rotator back to
the optical polarization beam splitter by transmitting through the
Faraday rotator for a second time; and a fiber delay line between
an optical path between the optical polarization beam splitter and
the reflective unit to transport light. The optical polarization
beam splitter is coupled to the optical loop to direct light
reflected back from the reflective unit into the optical loop.
[0010] This application also describes opto-electronic oscillators
that include a laser to produce CW laser light; an optical
modulator to modulate the CW laser light to produce modulated laser
light in response to an electrical control signal; an optical
splitter to receive at least a portion of the modulated laser light
and to split the received portion into a first beam and a second
beam; a first optical delay path to receive the first beam; a
second optical delay path to receive the second beam, wherein the
first and second optical paths have different optical delays; a
photodetector which is coupled to receive the first and second
beams, at orthogonal polarizations, from the first and second
optical delay paths to produce a detector signal; and an electrical
section operable to receive and process the detector signal to
produce the electrical control signal. The electrical section, the
optical modulator, the optical splitter, the first and second
optical delay paths, and the photodetector form a part of a closed
opto-electronic feedback loop that is operable to have a loop gain
greater than the loop loss and to generate an oscillation at a
modulation frequency of the optical modulator.
[0011] These and other implementations and other features are
described in greater detail in the drawings, the detailed
description and the claims.
BRIEF DESCRIPTION OF DRAWINGS
[0012] *FIGS. 1, 2 and 3 show examples of coupled opto-electronic
oscillators that use a dispersion compensation mechanism and a
polarization control mechanism to achieve a shortened optical loop
and a low phase noise.
[0013] FIGS. 4A and 4B show two implementations of a fiber Bragg
grating dispersion compensator in the device in FIG. 3.
[0014] FIGS. 5 and 6 show two implementations of coupled
opto-electronic oscillators that use a polarization beam splitter
and a Faraday rotator to control the polarization inside the
optical loop and to reduce the polarization-sensitive optical
loss.
[0015] FIGS. 7A and 7B show two example of coupled opto-electronic
oscillators that use an optical resonator to replace an optical
fiber delay line.
[0016] FIGS. 8, 9A, 9B and 9C show examples of coupled
opto-electronic oscillators that two different optical paths and a
single optical detector in the opto-electronic feedback loop to
achieve improved oscillator performance.
[0017] FIG. 10 shows a measured frequency spectrum of the COEO
shown in FIG. 9A with two optical paths and a single optical
detector in the opto-electronic feedback loop.
[0018] FIG. 11 shows one exemplary OEO in a non-COEO configuration
where the design shown in FIG. 9A is used for the two optical delay
paths and the single optical detector.
[0019] FIG. 12 shows a measured frequency spectrum of the OEO in
FIG. 11 with two optical paths and a single optical detector in the
opto-electronic feedback loop.
DETAILED DESCRIPTION
[0020] An OEO may be configured as a coupled opto-electronic
oscillator (COEO) which directly couples a laser oscillation in an
optical feedback loop (e.g., a laser cavity) to an electrical
oscillation in an opto-electronic feedback loop. See, e.g., U.S.
Pat. No. 5,929,430 which describes some examples of COEOs and is
incorporated by reference in its entirety as part of this
application. The laser oscillation and the electrical oscillation
are correlated with each other so that both the modes and stability
of one oscillation are coupled with those of the other oscillation.
The optical feedback loop includes an optical gain medium (i.e.,
laser medium) and is a positive feedback loop to produce a
sufficient optical gain greater the total optical loss to
effectuate the laser oscillation in the optical feedback loop. This
optical loop may be in a Fabry-Perot resonator, a ring resonator,
and other optical resonator configurations. The optical gain medium
may be excited or energized by an optical pump beam such as an
ion-doped fiber optical amplifier or by an electrical source such
as a semiconductor optical amplifier (SOA) excited by an electrical
driving current. Multiple optical modes (i.e., the longitudinal
modes) of the laser feedback loop can exist and the optical mode
spacing of two adjacent optical modes spacing is determined by the
optical length of the optical loop and is inversely proportional to
the optical length of the optical loop. These optical modes tend to
be independent from one another in phase. Hence, in absence of the
opto-electronic feedback loop, the laser oscillation may occur at
multiple optical modes and is a continuous wave (CW) laser
oscillation.
[0021] The opto-electronic loop in COEO is configured as a positive
feedback loop and has a total loop gain greater than the total loop
loss to sustain the electrical oscillation. The coupling between
two feedback loops is achieved by an optical modulation of an
optical parameter of the optical loop (e.g., the optical gain or
loss) at a modulation frequency equal to the oscillation frequency
of the opto-electronic feedback loop. The electrical signal in the
opto-electronic feedback loop is applied as a control signal to
control the optical modulation. This optical modulation modulates
each optical mode to create modulation sidebands on both sides of
each optical mode. This optical modulation can cause mode locking
of different optical modes in the optical loop when the modulation
frequency is equal to the optical mode spacing or a multiplicity of
the optical mode spacing of the optical modes in the optical loop
because the sidebands of each modulated mode coincide with its
neighboring bands. The mode locking causes the laser light to be an
pulsed output in the time domain. After the mode locking is
established, the actual mode spacing of the laser oscillation is
equal to the frequency of the opto-electronic loop.
[0022] Therefore, the laser oscillation and the electrical
oscillation in the COEO are correlated with each other in a way
that the gain in the electrical oscillation in the opto-electronic
feedback loop is partially obtained from the optical gain in the
optical loop and the phase noise of the electrical oscillation can
be suppressed via a long optical delay in the optical portion of
the opto-electronic loop. Accordingly, the electrical oscillation
in the COEO can exhibit a high quality factor and a low phase noise
level that are difficult to achieve with other RF oscillators
without the oscillating opto-electronic feedback loop. Some
applications require a low phase noise of about or less than -140
dBc/Hz at 10 kHz offset and the corresponding length of the fiber
for a sufficiently long delay in a COEO is on the order of several
kilometers.
[0023] The optical portion of the opto-electronic feedback loop
includes at least the optical loop and may also include an
additional optical delay line that separate from the optical loop
to further cause delay for an optical signal extracted out of the
optical loop. When the optical loop for the laser oscillation is
used as the primary source for the long optical delay in order to
decrease the phase noise, the spacing of the optical modes in the
laser oscillation is small. In a COEO which oscillates at a
frequency equal to a multiplicity of the optical mode spacing, an
optical mode that does not coincide with an oscillation mode of the
opto-electronic feedback loop may not be completely suppressed by
the mode matching in the coupled optical loop and the
opto-electronic loop and thus may be present as a spurious mode in
the spectrum of the electrical oscillation signal. When the optical
loop is a fiber ring to form a ring laser, an acceptable phase
noise level in such a COEO in some application corresponds to a
fiber length for the ring of about a few kilometers, e.g., 2 km. A
2-km fiber loop creates an optical mode spacing of about 100 kHz.
For an RF oscillation at 1 GHz, a spurious mode at 100 kHz from the
RF away the RF carrier may impose serious technical difficulties in
device designs (e.g., difficulty in RF signal filtering) and device
performance in some applications.
[0024] Therefore, it is desirable to design the COEO with a short
optical loop for the laser oscillation in order to create a
sufficiently large optical mode spacing for the optical modes in
the laser oscillation so that the spurious modes are spaced with a
sufficiently large frequency separation from an RF carrier in the
electrical oscillation signal. This use of a short optical loop for
the laser oscillation apparently is in conflict with the need for a
long optical delay in the opto-electronic feedback loop to reduced
the phase noise the electronic oscillation signal.
[0025] The above seemingly conflicting requirements for the optical
length of the optical loop in the COEO, however, can be resolved by
properly designing the optical components of the COEO. The low
phase noise performance of a long optical loop in the COEO is at
least in part contributed by the effective high quality Q factor of
the optical loop. The high Q factor of the optical loop can be
achieved by using a shorter optical loop by reducing optical loss
in the optical loop. As an example, one cause for the optical loss
in the optical loop in the COEO is the optical dispersion which
increases the phase between optical modes, resulting in spreading
and widening of the short optical pulse and reduction of the mode
locking efficiency. Thus, the optical dispersion reduces the
effective Q factor of the optical loop. In previous COEO designs
using a fiber ring to construct the optical loop for generating the
laser oscillation, the optical dispersion of the fiber was not
addressed. The reduction in Q enhancement caused by the optical
dispersion was offset by--using a long fiber ring with a large
optical delay.
[0026] One way to address the above seemingly conflicting
requirements for the optical length of the optical loop in the COEO
is to provide a dispersion compensation mechanism in the optical
loop for the laser oscillation so that a high quality Q factor can
be achieved with a shorter optical length for the optical loop in
comparison with an optical loop of a similar loop construction
without the dispersion compensation mechanism. This use of the
dispersion compensation mechanism in the optical loop of the COEO
can be used to achieve a desired large optical mode spacing of the
optical loop while still maintaining a desired low phase noise
level and a high Q factor for the COEO.
[0027] FIG. 1 shows one implementation of a COEO 100 using a
dispersion compensated ring laser design for a closed optical loop
that internally produces an optical gain. The COEO 100 includes an
optical fiber ring 101 and an opto-electronic feedback loop 102
which contains the fiber ring 101 as part of its optical portion.
The ring 101 forms a ring laser and includes an optical modulator
110, an optical gain medium or optical amplifier 112, and an
optical coupler 120 for producing an optical feedback signal from
the laser light in the ring 101. An optical filter 118 may also be
included in the ring 101. The optical modulator 110 is operable to
performs an optical modulation to cause the mode locking of
different longitudinal modes of the ring cavity and may an
amplitude modulator or a phase modulator. An opto-electronic
feedback loop 102 is formed in the COEO 100 by the optical fiber
ring 101, the optical coupler 120, an optical path to receive the
coupled optical feedback signal, an optical detector or
photodetector (PD) 130 to covert the optical feedback signal into
an electrical signal and an electrical portion to produce an
electrical control signal form the electrical signal output by the
optical detector 130 to control the optical modulator 110. In the
illustrated example, the photodetector 130 is the interface between
the optical portion and the electrical portion of the
opto-electronic feedback loop. The electrical portion of the
opto-electronic feedback loop 102 includes RF amplifiers 132 and
136 to amplify the signal and an RF filter 134 to filter the
signal. In some implementations, a variable signal phase shifter
138 (e.g., a voltage-controlled RF phase shifter) or an RF line
stretcher may be included in the electrical portion to adjust the
phase of the control signal to the optical modulator 110 so that
the proper mode matching condition is met by overlapping an
oscillation mode of the opto-electronic feedback loop 102 with an
optical mode of the optical loop 101 and to ensure that the control
signal is a positive feedback to initiate and sustain the
opto-electronic oscillation. Other OEOs and COEOs described in this
application can also include such a phase shifter 138.
Alternatively, the phase delays in the COEO can be predetermined
and fixed in the final COEO to ensure the proper feedback phase in
the opto-electronic feedback loop and the proper mode matching
condition. An RF signal coupler 140 may also be included in the
electrical portion of the opto-electronic feedback loop to output
the electronic oscillation signal of the COEO 100. In operation,
the opto-electronic feedback loop 102 uses at least one portion of
the laser light generated in the optical ring 101 to generate the
control signal for controlling the optical modulator 110.
[0028] The optical fiber ring 101 can include a length of single
mode fiber (SMF) 114 to which various optical elements in the ring
are coupled. This fiber may be a polarization maintaining (PM)
fiber. Notably, a dispersion compensation element 119 is included
in the fiber ring 101 to produce optical dispersion that negates
the optical dispersion present in the ring 101 so that the net
optical dispersion in the ring 101 is minimized and the optical
length of the ring 101 can be shortened to achieve a desired large
optical mode spacing. The dispersion compensation element 119 may
be implemented in various configurations, including a dispersion
compensation fiber (DCF), a dispersion shifted fiber, and a fiber
Bragg grating dispersion compensator.
[0029] In the specific example in FIG. 1, a segment of single mode
fiber of 260 meters using the Corning SMF28 fiber is used as the
fiber 114 to form the fiber ring 101. The dispersion compensation
element 119 is a segment of dispersion compensation fiber (DCF) of
40 meters and is spliced to the fiber 114. The lengths of the fiber
segments 114 and 119 used in this example are determined based on
the desired total optical length of the fiber ring 101 for the
optical mode spacing and the need to minimize the total optical
dispersion in the ring 101. The DCF is effectively an additional
length of a different fiber with abnormal dispersion that negates
the dispersion in the fiber ring. The exact length of DCF can be
calculated based on the characteristics of the main fiber. This
design may be performed in two steps. First, the length of the
optical ring is initially designed to be sufficiently short to
achieve the minimum separation between the carrier and the first
spurious mode. Next, based on the set short length of the optical
ring, the dispersion compensation element is designed to compensate
for the dispersion in the fiber ring to reduce the phase noise
below an acceptable level that can be otherwise achieved with a
longer length for the optical ring. This approach is based on the
fact that if the chromatic dispersion of the fiber is compensated
then the dispersion-compensated fiber's behavior in phase noise is
effectively like a longer fiber in an active lasing system like the
optical ring in FIG. 1. This dispersion compensated fiber ring can
produce a Q factor similar to that of a fiber ring of about 4 km
(or longer) formed with the Corning SFM 28 fiber without dispersion
compensation. The addition of the dispersion compensation element
in the optical ring does not significantly change the frequency
spacing between the carrier and the first spurious mode, which is
dictated by the shorted length of the optical ring.
[0030] FIG. 2 shows an implementation of the COEO in FIG. 1, where
two semiconductor amplifiers 210 and 220 are used as the optical
gain medium 112 in FIG. 1 to generate laser light. An optical
bandpass (PB) filter (e.g., with a transmission band of 5 nm) is
used to implement the filter 118 to suppress light and optical
noise outside the laser frequency. In both FIGS. 1 and 2, the
optical modulator 110 is a separate device from the optical gain
medium (SOAs in this example) and modulates the laser light
generated in the optical ring at an oscillation frequency below the
optical spectrum, e.g., a RF or microwave frequency. Alternatively,
the optical modulator 110 may be a SOA to both amplify laser light
and to modulate the laser light in the fiber ring 101. The optical
coupler 120 may be an optical splitter such as a 90/10 optical
splitter as shown.
[0031] The dispersion compensation element 119 in FIGS. 1 and 2 may
also be implemented by one or more fiber Bragg grating (FBG)
dispersion compensators in the optical ring 101 for dispersion
compensation. A fiber Bragg grating compensator may be formed in a
PM fiber that is used to form the optical ring 101 in the COEO in
FIG. 1 or 2. The fiber Bragg grating may have a spatially chirped
grating period along the grating to produce different dispersions
at different wavelengths to negate the dispersion in the fiber ring
101. In addition to dispersion compensation, the fiber Bragg
grating itself can also operate as an optical wavelength filter and
thus eliminates the need for a separate optical filter in the loop
101.
[0032] FIG. 3 illustrates a COEO that is based on the design in
FIG. 1 and implements a FBG dispersion compensator 310 in the ring
101. FIG. 4A further shows one implementation of the FBG dispersion
compensator 310 which includes an optical circulator 410 and a
fiber Bragg grating 420. The circulator 410 is connected to receive
light out of the fiber delay line 114 and directs the received
light into the fiber Bragg grating 420. The fiber Bragg grating 420
reflects the light from the circulator 410 to produce reflected
light with reduced dispersion. The reflected light is received by
the circulator 410 and is directed back into the fiber ring 101.
FIG. 4B shows a different implementation where the fiber delay line
114 is coupled between the optical circulator 410 and the fiber
Bragg grating 420. The fiber Bragg grating 420 in both
implementations is configured to minimize the dispersion on the
light that is coupled back to the ring 101.
[0033] In the COEOs in FIGS. 1-3 and other configurations, a
certain part of the optical loop 101 can be sensitive to optical
polarization and thus may experience polarization-dependent optical
loss if the polarization is not at a particular polarization state.
For example, the optical modulator 110 and the optical gain medium
112 in the COEOS in FIGS. 1-3 may be sensitive to polarization of
light. This polarization-dependent optical loss contributes to the
overall optical loss in the optical loop 101 and thus can reduce
the effective Q factor of the optical loop and the COEO. Therefore,
a polarization control mechanism may be implemented in the COEO to
reduce the optical loss in the optical loop 101 and to enhance the
effective Q factor of the COEO. The polarization control mechanism
may be implemented either in a combination with the dispersion
compensation in a COEO or without the dispersion compensation.
[0034] The COEOS in FIGS. 1-3 show a polarization controller 116
coupled in the optical loop 101 to control the polarization of the
light in the ring 101, thus minimizing the polarization-sensitive
optical loss. In operation, the polarization controller 116 is
adjusted to minimize the overall optical loss in the fiber ring
101. In some implementations, each polarization-sensitive location
in the fiber ring 101 may include a designated polarization
controller to ensure the proper polarization at that location,
e.g., one at the entrance of the optical modulator 110 and another
at the entrance of the optical amplifier 112.
[0035] FIG. 5 shows an alternative implementation where the fiber
ring 101 is constructed by using PM fiber which is coupled to each
polarization-sensitive component in the ring 101 to minimize the
polarization-sensitive loss locally. For optical components in
which the polarization of light is difficult to control, the COEO
in FIG. 5 places these non-PM optical components between a
polarization beam splitter (PBS) 510 and a Faraday rotator 521 to
optically isolate these non-PM optical components from each optical
path where the polarization of light is required to be maintained
at a certain polarization state and thus to minimize effects of
these optical components on each of the polarization sensitive
components in the ring 101.
[0036] As an example, many commercial single mode dispersion
compensation fibers are not PM fibers. Therefore, the single mode
fiber delay line 114 and the DCF 119 in FIGS. 1 and 2 may not
maintain the polarization of light. The COEO in FIG. 5 places the
single mode fiber delay line 114 and the DCF 119 between the PBS
510 in the ring 101 and a Faraday rotor mirror (FRM) 520 off the
main PM fiber portion of the ring 101. The FRM 520 includes a
45-degree Faraday rotator 521 and a mirror 522. Light from the PBS
510 first transmit through the Faraday rotator 521 and is reflected
by the mirror 522 to transmit the Faraday rotator 521 for the
second time and is rotated by 90 degrees in polarization with
respect to the incident polarization from the PBS 510. The PBS 510
has three ports 1, 2 and 3, respectively. The input port 1 is
coupled to the PM fiber in the ring 101 so that the polarization
(P1) aligned with the PM direction of the PM fiber is directed to
the second port 2 (e.g., reflected to the port 2 by a polarization
sensitive reflecting surface) as light in a polarization P2 which
is the same as P1. The light output from the port 2 passes through
the single mode fiber delay line 114 and the DCF 119 and is
reflected back (Pr) by the Faraday rotator mirror 520 to be
orthogonal to the incident polarization at each location between
the PBS 510 and the Faraday rotator mirror 520. Therefore, the
polarization (Pr) of the light reflected back to the PBS 510 at the
port 2 is orthogonal to the polarization (P2) of light output at
the port 2 by the PBS 510. Accordingly, the reflected light
transmits through polarization sensitive reflecting surface of the
PBS 510 to the port 3. The port 3 is coupled to the PM fiber in the
ring 101 so that the polarization of light output at the port 3 is
along the PM direction of the PM fiber in the ring 101. With
reference to the polarization direction of the PBS 510, the two PM
fiber segments respectively coupled to the ports 1 and 3 are
oriented 90 degrees relative to each other.
[0037] Hence, the portion of the ring 101 between the BPS 510 and
the FRM 520 is the non-PM portion of the ring and the rest of the
ring 101 is the PM portion due to the use of PM fiber. In
operation, light in the ring 101 is directed out of the PM portion
of the ring 101 via the port 1 of the PBS 510 to the elements 114,
119 and 520 and is directed back into the PM portion of the ring
101. This design isolates any variation in the polarization of
light in the non-PM portion between the PBS 510 and the FMR 520
from affecting the light polarization in the PM portion of the ring
101 because the light that is coupled back the PM portion by the
port 3 of the PBS 510 is always aligned to the PM direction of the
PM fiber. Notably, the light passes through the single mode fiber
delay line 114 and the DCF 119 twice in one roundtrip in the ring
101 so that effect on the light by each of the single mode fiber
delay line 114 and the DCF 119 is doubled. This allows the length
of each of the single mode fiber delay line 114 and the DCF 119 to
be reduced by one half in comparison of the designs in FIGS. 1 and
4 where light only passes through the single mode fiber delay line
114 and the DCF 119 only once in one roundtrip in the ring 101.
[0038] FIG. 6 shows a variation of the design in FIG. 5 where the a
reflective Fiber Bragg grating 610 is used to replace the DCF 119
and the mirror 522 in FIG. 5. The fiber Bragg grating 610 is placed
at the location of the mirror 522 to reflect light back and to
produce negating dispersion that reduces the overall dispersion in
the ring 101.
[0039] In the above examples, the optical fiber delay line 114 is
used to produce the majority of the optical delay in the
opto-electronic feedback. A high-Q optical resonator may be used to
replace the optical fiber delay line 114 in the above and other
implementations described in this application. Examples of COEOs
using an optical resonator as an optical delay and their operations
are described in U.S. Pat. No. 6,567,436 entitled "OPTO-ELECTRONIC
OSCILLATORS HAVING OPTICAL RESONATORS" which is incorporated by
reference as part of the specification of this application. Such an
optical resonator is an integral part in the optical portion of the
opto-electronic feedback loop to provide a sufficiently long energy
storage time and hence to produce an oscillation of a narrow
linewidth and low phase noise. The mode spacing of the optical
resonator is equal to one mode spacing, or a multiplicity of the
mode spacing, of the opto-electronic feedback loop. In addition,
the oscillating frequency of the COEO is equal to one mode spacing
or a multiple of the mode spacing of the optical resonator.
Furthermore, the laser center frequency V.sub.laser of the laser
light in the optical loop 101 is within one of the transmission
peaks of the optical resonator. This optical resonator can also
operate as an optical bandpass filter and the separate filter 118
may be eliminated from the ring 101. The optical resonator may be
implemented in a number of configurations, including, e.g., a
Fabry-Perot resonator, a fiber ring resonator, a
whispering-gallery-mode microsphere resonator, a
whispering-gallery-mode microdisc resonator, a
whispering-gallery-mode microresonator in a non-spherical
geometry.
[0040] FIGS. 7A and 7B show two examples COEOS based on the COEOs
in FIGS. 1 and 5, respectively. An optical resonator 701 is used to
replace the fiber delay line 114. This technique can also be
applied to other COEOs and their variations based on the
specification of this application.
[0041] The above COEOs use a single opto-electronic feedback loop.
In other implementations, the optical section of the single
opto-electronic feedback loop may include two different optical
paths with different optical delays to form a dual loop
configuration to further restrict the optical mode selection and to
reduce the number of spurious modes at the optical modes that are
not selected for the laser oscillation in the COEO. Certainly,
three or more optical paths may be used to form a multi-loop
configuration to further eliminate the number of optical modes in
the COEO. This use of two or more optical paths with different
optical delays can improve the oscillator performance. U.S. Pat.
No. 5,777,778 entitled "MULTI-LOOP OPTO-ELECTRONIC MICROWAVE
OSCILLATOR WITH A WIDE TUNING RANGE" describes examples of
multiloop OEOs and is incorporated by reference as part of the
specification of this application. The different feedback loops in
an OEO or COEO have different delays. The opto-electronic feedback
loop with the longest delay is used to achieve low phase noise and
narrow spectral linewidth. This loop is also used to provide fine
frequency tuning since its mode spacing is smaller than any of the
other feedback loops. On the other hand, the feedback loop with the
shortest delay and the widest mode spacing is used to provide a
coarse frequency tuning to achieve a wide continuous tuning range.
The total open loop gain of the multiple loops must exceed the
total losses to sustain an opto-electronic oscillation but each
loop may have an open loop gain less then the loss in that
loop.
[0042] FIG. 8 illustrates one example of a COEO based on the design
in FIG. 5 to show an example of an opto-electronic feedback loop
with two optical paths in the optical portion of the feedback loop.
In this configuration, an optical coupler 801 is used to split the
output of the laser light into two beams into two different optical
delay lines 810 and 820, respectively. The two optical beams out of
the two optical delay lines 810 and 820 are then combined at a
single optical detector 130 which converts the combined optical
signal into an electrical signal for processing by the electrical
portion of the feedback loop. A polarization control mechanism is
provided to make the two optical beams from two optical paths to be
orthogonal to each other and thus the two beams at the optical
detector 130 do not optically interfere. Accordingly, the
electrical output of the optical detector 130 is a simple sum of
the two delayed signals from the two optical paths 810 and 820.
Notably, this design eliminates the optical interference between
the two signals from the two optical paths but still allows for RF
or microwave interference that leads to the improved oscillator
performance.
[0043] In comparison with a multi-loop OEO or COEO that provides
different optical paths with different optical detectors, the
single-detector design in FIG. 8 keeps the number of the optical
detectors at the minimum (i.e., only one detector) and thus reduces
the circuit complexity, size and cost. The optical mode selection
and optical filtering provided by the two or more different optical
paths also relax the requirements of the electrical filtering with
respect to at least the filtering bandwidth of an electrical filter
in the electrical portion of the opto-electronic loop by allowing
an RF filter with a relative wide bandwidth to be used without
comprising the ability to achieve a narrow linewidth in the RF
oscillation signal. These features are particular significant in
integrated COEOs where various optical and electronic components
are integrated on a common substrate.
[0044] FIGS. 9A, 9B and 9C illustrate three different
implementations of two optical paths and a single optical detector
as shown in FIG. 8. In FIG. 9A, each optical path is formed with a
PM fiber and the two different optical delay paths 810 and 820 have
orthogonal polarizations. A PBS 910 is used as an optical
polarization-sensitive combiner to combine the two orthogonally
polarized beams into a single beam for detection at the single
optical detector 130. In FIG. 9B, the optical paths use non-PM
fibers such as single mode fibers and at least one polarization
controller used in one of the two optical delay paths to ensure the
two beams to be orthogonal to each other at the single optical
detector 130. A polarization-insensitive optical coupler may be
used to combine the two beams before the optical detector 130. In
FIG. 9C, a PBS 930 is used as the optical coupler 801 to split the
input light to the optical portion of the opto-electronic feedback
loop into two orthogonally polarized beams. This may be achieved by
orientating the polarization direction of the PBS 930 to be at an
angle of 45 degrees with respect to the polarization of the input
light. The two different optical paths are formed with PM fibers to
maintain their respective polarizations. FIG. 10 shows a measured
frequency spectrum of the COEO shown in FIG. 9A with two optical
paths and a single optical detector in the opto-electronic feedback
loop. The two optical delay paths use two PM fiber paths of 1 m and
650 m, respectively. The optical loop of COEO includes a single
mode fiber of 1 km by using Corning's SFM-28 fiber. The RF filter
used in the opto-electronic feedback loop has a bandwidth of 350
MHz. This COEO is functionally equivalent to a COEO with two
separate loops of 1.65 km and 1 km in length, respectively.
Notably, the RF oscillation signal near 9.7 GHz has a linewidth
much narrower than the bandwidth of 350 MHz of the RF filter used
in the electrical portion of the feedback loop.
[0045] The designs of using multiple optical delay paths with a
single optical detector in the opto-electronic feedback loop shown
in FIGS. 8, 9A, 9B and 9C may be applied to other OEOs. FIG. 11
shows one exemplary OEO in a non-COEO configuration where the
design shown in FIG. 9A is used for the two optical delay paths and
the single optical detector. A laser 1101 is used to provide a CW
laser beam into a PM fiber path 1104. An optical modulator 1110,
which may be either an amplitude modulator or a phase modulator, is
used to modulate the CW laser beam from the laser 1102 to produce a
modulated beam in response to an electrical control signal from the
opto-electronic feedback loop. A PM fiber path 1106 is provided to
receive the modulated beam to the two optical delay paths 810 and
820. A fiber delay line 1130 of length L3 is placed between the PBS
910 and the single optical detector 130 to introduce an additional
delay to the loop. This delay line 1130 may be replaced by an
optical resonator as described above. The detector output from the
detector 130 is electronically processed by the electrical portion
of the loop to produce the electrical control signal applied to the
optical modulator 1110. Alternatively, the OEO in FIG. 11 may be
modified to use the configurations shown in FIGS. 9B and 9C for the
two optical delay paths and the single optical detector.
[0046] FIG. 12 shows a measured frequency spectrum of the OEO in
FIG. 11 with two optical paths and a single optical detector in the
opto-electronic feedback loop. The RF filter used in the
opto-electronic feedback loop has a bandwidth of 360 MHz. Once
again, the RF oscillation signal has a linewidth much narrower than
the bandwidth of 360 MHz of the RF filter used in the electrical
portion of the feedback loop.
[0047] The above described COEOs and OEOs may be configured as
fixed oscillators which produce fixed oscillation frequencies in RF
or microwave ranges or as tunable oscillators to tune the
oscillation frequencies in response a control signal. A tunable
COEO or OEO may be tuned by using a tunable optical delay device in
the optical portion in the COEO or OEO, such as a fiber stretcher
in a fiber delay line or a tunable optical resonator that is used
as an optical delay element. An electro-optic material may be used
in an optical resonator to make it tunable. A tunable COEO or OEO
may also be tuned by using a tunable electrical device in the
electrical portion of the opto-electronic feedback loop such as a
variable RF delay device or a voltage controlled RF phase shifter.
An OEO or COEO may also be tuned by using both an optically tunable
device and an electrically tunable device.
[0048] In summary, only a few implementations are disclosed.
However, it is understood that variations and enhancements may be
made.
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